2020
DOI: 10.1103/physrevb.102.045433
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Self-duality triggered dynamical transition

Abstract: A basic result about the dynamics of spinless quantum systems is that the Maryland model exhibits dynamical localization in any dimension. Here we implement mathematical spectral theory and numerical experiments to show that this result does not hold, when the 2-dimensional Maryland model is endowed with spin 1/2 -hereafter dubbed spin-Maryland (SM) model. Instead, in a family of SM models, tuning the (effective) Planck constant drives dynamical localization-delocalization transitions of topological nature. Th… Show more

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Cited by 6 publications
(9 citation statements)
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References 48 publications
(89 reference statements)
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“…Similar notions of dualities were suggested in systems ranging from self-assembled systems [10] to quantum rotors [11]. Rich consequences arise when a duality is combined with other constraints such as symmetries or conservation laws, ranging from degeneracies in the band structure [12][13][14] and topological states [15,16] to symmetries in the phonon response [17] and constraints on the stiffness tensor of an elastic medium [18].…”
Section: Introductionmentioning
confidence: 71%
“…Similar notions of dualities were suggested in systems ranging from self-assembled systems [10] to quantum rotors [11]. Rich consequences arise when a duality is combined with other constraints such as symmetries or conservation laws, ranging from degeneracies in the band structure [12][13][14] and topological states [15,16] to symmetries in the phonon response [17] and constraints on the stiffness tensor of an elastic medium [18].…”
Section: Introductionmentioning
confidence: 71%
“…Moreover, the phases encoded in these amplitudes have to be considered simultaneously to correctly trace the quantum evolution. (10)]. The green triangles, the red circles, and the blue squares are for the quantum results with j = 100, 200, and 400, respectively.…”
Section: B the Pseudoclassical Limit Of The Kicked Topmentioning
confidence: 99%
“…For the two cases close to the quantum resonance condition discussed in the previous section, we can see immediately how their linear entropy is related to that of the case β = δ based on the pseudoclassical analysis. First, for β = 2jπ + δ, from Equation (10), we have that [J γ (n; β)] 2 = [J γ (n; δ)] 2 at any time n; hence, S(n) must coincide with that for the system of β = δ throughout. However, for β = jπ + δ, from Equation ( 12), we know that γ [J γ (n; β)] 2 = γ [J γ (n; δ)] 2 only when mod (n, 8) = 0 or 4.…”
Section: The Dynamical Entanglementmentioning
confidence: 99%
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